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SOLUTIONSMANUAL TO ACCOMPANY ATKINS' PHYSICAL CHEMISTRY 25 With the data given b = Vm − RTV 2m pV 2m + a = (4.00 × 10−4 m3mol−1) − (8.3145 JK−1mol−1) × (288 K) × (4.00 × 10−4 m3mol−1)2 (4.0 × 106 Pa) × (4.00 × 10−4 m3mol−1)2 + (0.76 m6 Pamol−2) = 1.3 × 10−4 m3mol−1 where 1 Pa = 1 kgm−1 s−2 and 1 J = 1 kgm2 s−2 have been used. �e compression factor Z is de�ned in [1C.1–20] as Z = Vm/V○m, where V○m is the molar volume of a perfect gas under the same conditions. �is volume is computed from the equation of state for a perfect gas, [1A.4–8], as V○m = RT/p, hence Z = pVm/RT , [1C.2–20]. With the data given Z = pVm RT = (4.0 × 106 Pa) × (4.00 × 10−4 m3mol−1) (8.3145 JK−1mol−1) × (288 K) = 0.67 Solutions to problems P1C.2 (a) Using the perfect gas law, pV = nRT , the molar volume is calculate as Vm = RT p = (8.2057 × 10−2 dm3 atmK−1mol−1) × (350 K) 2.30 atm = 12.5 dm3mol−1 (b) �e van derWaals equation of state in terms of the molar volume is given by [1C.5b–24], p = RT/(Vm−b)−a/V 2m; the term a/V 2m is due to attractive interactions. �is equation is a cubic inVm which can be solved numerically. A simpler approach is to approximate a/V 2m as a/(V○m)2, where V○m is the molar volume of a perfect gas under the prevailing conditions. �e van der Waals equation is then rearranged to give a simpler expression for Vm p = RT (Vm − b) − a (V○m)2 hence Vm = RT p + [a/(V○m)2] + b �e van der Waals constants for Cl2 are a = 6.260 atmdm6mol−2 and b = 5.42 × 10−2 dm3mol−1. With these values, the �rst approximation to the molar volume is calculated as Vm = (8.2057 × 10−2 dm3 atmK−1mol−1) × (350 K) (2.30 atm) + [(6.260 atmdm6mol−2)/(12.5 dm3mol−1)2] + 5.42 × 10−2 dm3mol−1 = 12.3 dm3mol−1 �is approximate value forVm is then used in place ofV○m and the process repeated, to give Vm = 12.3 dm3mol−1 – the same value.�e process has converged (to this level of precision).